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Analytical Chemistry Chemical Cytometry Quantitates Superoxide

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Switzerland), was placed inside the chromatographic oven to<br />

bypass the combustion furnace when required. The valve has an<br />

extension between the body and the actuator which allows the<br />

valve to be mounted in the heated zone while the handle remains<br />

outside at ambient temperature. This valve prevented the solvent<br />

from entering the combustion unit and therefore enlarged the<br />

catalytic activity of the Cu and Pt wires. Additionally, the valve<br />

allowed the direct connection of the column with the EI source<br />

for conventional GC-MS work in order to identify the different<br />

species under analysis by their fragmentation pattern. Moreover,<br />

such qualitative analysis is essential to assess peak purity for each<br />

compound. For postcolumn isotope dilution analysis the valve was<br />

initially in the “load” position (combustion oven bypassed) and<br />

the valve was manually switched to the “inject” position at the<br />

same time that the EI filament switched on. All connections<br />

between the valve and the rest of the components of the system<br />

were performed by means of 0.32 mm i.d. deactivated fused silica<br />

capillaries and fixed to the valve with appropriate polyimide coated<br />

fused silica adapters (VICI AG International, Schenkon, Switzerland).<br />

Combustion Furnace. The laboratory-made combustion furnace<br />

consisted of a 60 cm long ceramic tube (3 mm O.D., 0.5 mm I.D.)<br />

(Elemental microanalysis, Devon, U. K.) filled with copper and<br />

platinum wires and heated by a Nichrome wire. Proper thermal<br />

isolation of the combustion furnace was provided with glass wool.<br />

The combustion furnace was set vertically on top of the GC with<br />

the lower end of the ceramic tube inside the chromatographic<br />

oven to avoid cold spots after the separation. High temperatures<br />

were accurately controlled using a temperature sensor and an<br />

external controller, allowing temperature settings inside the tube<br />

to be within ±1 °C over a wide temperature range (50-1200 °C).<br />

The copper wires were previously oxidized by passing an oxygen<br />

flow (1 mL/min) at 450 °C during 4-5 h and this procedure was<br />

performed on a weekly basis to preserve its oxidizing capabilities.<br />

Fused silica capillaries (0,32 mm i.d.) were used to connect the<br />

furnace to the valve and to the ion source respectively. For this<br />

purpose a length (∼1 cm) at one end of each capillary was<br />

uncoated, to prevent the polyimide coating to be burnt, and<br />

introduced into the ceramic tube. Reducing unions 1/8′′ to 1/16′′<br />

(SGE, Victoria, Australia) and appropriate graphite ferrules (0.5<br />

mm i.d.) were used to hold the capillaries in place at both sides<br />

of the ceramic tube. For oxidation and combustion, the furnace<br />

was operated at 850 °C.<br />

Gas Cylinder and Mass Flow Controller. The 13 CO2 container<br />

was a dual inlet 5 L high pressure stainless steel gas cylinder<br />

(Iberfluid, Barcelona, Spain). The cylinder was equipped on<br />

one end with, in this order, an opening valve, a Swagelok tee<br />

where helium could be introduced from a high pressure<br />

cylinder, and a second opening valve connected to the other<br />

end of the tee. This second valve was connected to a septum<br />

for the manual injection of gases into the cylinder. Before the<br />

cylinder was pressurized, 13 CO2 was injected into the container<br />

by means of a gastight syringe (Hamilton, Reno, U. S. A.)<br />

through this valve. After the injection of the tracer, the valve<br />

was closed and the container was pressurized up to 6 bar with<br />

helium using the connection in the Swagelok tee. When the<br />

set pressure was reached the filling valve was also closed. At<br />

the other end of the cylinder a pressure gauge, an opening<br />

6864 <strong>Analytical</strong> <strong>Chemistry</strong>, Vol. 82, No. 16, August 15, 2010<br />

valve and a mass-flow controller (Bronkhorst, Ruurlo, Netherlands)<br />

calibrated for He were coupled for the accurate control<br />

of the tracer flow. The opening valve was closed during the<br />

filling of the cylinder, remaining open the rest of the time. The<br />

flow rate for the postcolumn spike was set at 0.5 mL/min.<br />

Effluent and spike flows were mixed after combustion by means<br />

of a 0.25 mm bore stainless steel microvolume “Y” connector<br />

(VICI AG International, Schenkon, Switzerland).<br />

The whole instrumental setup is shown in Figure 1. As can be<br />

observed, the instrument can be operated in the standard GC-<br />

MS configuration (qualitative) or in the combustion-postcolumn<br />

configuration (quantitative) depending on the position of the<br />

switching valve.<br />

Procedures. Preparation of 13 CO2. The spike was prepared<br />

from 13 C enriched Na2CO3 (99%). An accurate weighed amount<br />

(∼200 mg) was placed in a 25 mL three-necked round-bottomed<br />

flask, previously purged with He to avoid natural abundances<br />

CO2 contamination from ambient air. A small quantity (300 µL)<br />

of concentrated H3PO4, was injected into the flask through a<br />

septum cap. After the acid-base reaction, 4 mL of the gaseous<br />

phase, containing 13 CO2 diluted in He, were removed using a<br />

gastight syringe and injected into the container shown in<br />

Figure 1.<br />

Calibration of the 13 CO2 Postcolumn Flow. The flow rate of<br />

the spike could be accurately controlled by the mass flow<br />

controller between 0.1 and 5 mL min -1 . In our experiments, it<br />

was set at 0.5 mL min -1 . The exact mass flow (ng of 13 CO2 per<br />

min) being mixed with the natural CO2 coming from the<br />

column and combustion furnace was determined by adding<br />

internal standards of known concentration spiked to the sample<br />

as described before. 11,15<br />

Quantification using Postcolumn Isotope Dilution. In our case,<br />

the isotope ratio 12 C/ 13 C was measured as the signal ratio at<br />

masses 44 and 45 (I44/I45) corresponding to the continuous<br />

blend of natural abundance 12 CO2 present in the chromatographic<br />

eluent and the enriched 13 CO2, added postcolumn.<br />

Selected Ion Monitoring (SIM) at masses 44.0 and 45.0 was<br />

performed for the duration of the chromatogram with 70 ms<br />

integration time per mass. The mass window was ∼0.1 mass<br />

units. Then, the isotope ratio in the blend, Rb ) I44/I45, was<br />

calculated to build the isotope ratio chromatogram (Rb vs time).<br />

The postcolumn isotope dilution equation, 7 shown as equation 1<br />

below, was then applied to every point in the chromatogram<br />

to obtain the mass-flow chromatogram (ng of C/min vs time).<br />

The integration of the mass flow chromatogram directly<br />

provided the amount of carbon (in ng) eluted in each chromatographic<br />

peak.<br />

MF n ) MF t<br />

AW n<br />

13<br />

At AWt An 12( Rb - Rt 1 - RbRn) In this equation MFn corresponds to the mass flow of carbon<br />

from the natural abundance sample injected, whereas MFt<br />

corresponds to the mass flow of carbon from the postcolumn<br />

spike or tracer. AWn and AWt correspond to the atomic weight<br />

of carbon in the sample and tracer, respectively. The isotope<br />

abundances At 13 and An 12 correspond to the isotopic composition<br />

of 13 C in the tracer and 12 C in the sample. Finally, Rt is the<br />

(1)

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